Beats — Question 8

Section 17-7 · Physics pages 2766–2767

Question 8 A short averaging window retains the beat cross term Two equal, nearly equal-frequency copropagating tones each have intensity I1. After averaging over rapid carrier cycles, their combined intensity is I(t) = 2I1[1 + cos(2π∆f t)], with phase alignment at t = 0. Average this expression over 0 ≤t ≤T. t I Carrier-averaged intensity oscillates at the beat rate; the averaging window selects part of this curve. (a) Derive the finite-window average. (b) Evaluate it for one full beat period and for one quarter of a beat period. Explain the long-window limit.
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Question 8 - Solution A short averaging window retains the beat cross term t I (a) Method and calculation Integrate the cross term explicitly: IT = 1 T ∫T 0 I(t) dt = 2I1 [ 1 + sin(2π∆fT) 2π∆fT ] . The starting phase matters for short windows; the supplied expression specifies that phase. (b) Interpretation and further calculation For T = 1/∆f, the sine term is zero and IT = 2I1. For T = 1/(4∆f), IT = 2I1(1 + 2/π) = 3.27324I1. As T∆f →∞, the bounded sine numerator divided by T vanishes. Long averaging removes the cross term and recovers the sum of individual intensities. Physical check The carrier averaging assumes many fast cycles within the time window while still allowing the beat envelope to vary slowly.

Question 8

A short averaging window retains the beat cross term

Two equal, nearly equal-frequency copropagating tones each have intensity I1I_1. After averaging over rapid carrier cycles, their combined intensity is I(t)=2I1[1+cos⁡(2πΔft)]I(t)=2I_1[1+\cos(2\pi\Delta f\,t)], with phase alignment at t=0t=0. Average this expression over 0≤t≤T0\le t\le T.

Diagram shown in the original SVG worksheet.

  1. Derive the finite-window average.

  2. Evaluate it for one full beat period and for one quarter of a beat period. Explain the long-window limit.

Question 8 - Solution

A short averaging window retains the beat cross term

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Integrate the cross term explicitly:I¯T=1T∫0TI(t)dt=2I1[1+sin⁡(2πΔfT)2πΔfT].\overline I_T=\frac1T\int_0^T I(t)\,dt=2I_1\left[1+\frac{\sin(2\pi\Delta f T)}{2\pi\Delta f T}\right].The starting phase matters for short windows; the supplied expression specifies that phase.

(b) Interpretation and further calculation

For T=1/ΔfT=1/\Delta f, the sine term is zero and I¯T=2I1\overline I_T=2I_1. For T=1/(4Δf)T=1/(4\Delta f),I¯T=2I1(1+2/π)=3.27324I1.\overline I_T=2I_1(1+2/\pi)=3.27324I_1.As TΔf→∞T\Delta f\to\infty, the bounded sine numerator divided by TT vanishes. Long averaging removes the cross term and recovers the sum of individual intensities.

Physical check

The carrier averaging assumes many fast cycles within the time window while still allowing the beat envelope to vary slowly.